A hybrid muon detector design with RPC and plastic scintillator for the experiment at the Super Tau-Charm Facility

2021 ◽  
Vol 16 (09) ◽  
pp. P09022
Author(s):  
Z. Fang ◽  
Y. Liu ◽  
H. Shi ◽  
J. Liu ◽  
M. Shao
Keyword(s):  
Plastic Scintillator ◽  
Muon Detector ◽  
Detector Design

A preliminary simulation study of influence of backsplash on the plastic scintillator detector design in HERD experiment

2021 ◽  
Author(s):  
Peng Hu ◽  
Zhi-gang Wang ◽  
Fabio Gargano ◽  
Francesca Alemanno ◽  
Corrado Altomare ◽  
...  
Keyword(s):  
Simulation Study ◽  
Plastic Scintillator ◽  
Scintillator Detector ◽  
Detector Design

scholarly journals MuCap: Muon Capture on the Proton

2021 ◽  
Author(s):  
Malte Hildebrandt ◽  
Claude Petitjean
Keyword(s):  
Time Projection Chamber ◽  
Plastic Scintillator ◽  
Capture Rate ◽  
Muon Capture ◽  
Recent Analysis ◽  
Muon Detector ◽  
Chiral Perturbation ◽  
Pseudoscalar Coupling ◽  
The Difference ◽  
Time Projection

The singlet muon capture rate \Lambda_SΛS on the proton \mu^-\ p \to \nu_\mu~nμ−p→νμn is determined in a high precision lifetime measurement. The main apparatus consists of a new hydrogen time projection chamber as muon detector, developed by PSI, surrounded by cylindrical wire chambers and a plastic scintillator hodoscope as electron detectors. The parameter \Lambda_SΛS is evaluated as the difference between the inverse \mu\,pμp lifetime and that of the free \mu^+μ+. The result \Lambda_S^\text{MuCap} = (715.6 \pm 5.4^\text{stat} \pm 5.1^\text{sys})\,\text{s}^{-1}ΛSMuCap=(715.6±5.4stat±5.1sys)s−1 is in excellent agreement with the prediction of chiral perturbation theory \Lambda_S^{\chi\text{PT}} = (715.4 \pm 6.9)\,\text{s}^{-1}ΛSχPT=(715.4±6.9)s−1. From \Lambda_S^\text{MuCap}ΛSMuCap a recent analysis derives for the induced pseudoscalar coupling g^\text{MuCap}_p = 8.23 \pm 0.83gpMuCap=8.23±0.83 whereas \bar{g}^{\chi\text{PT}}_p = 8.25 \pm 0.25g‾pχPT=8.25±0.25.

Proposal of a Novel Setup for Linac Monitoring Using a Specifically Designed Plastic Scintillator and a Spectrophotometer

2016 ◽  
Vol 4 (1) ◽  
pp. 175-182
Author(s):  
F. Moreno-Barbosa ◽  
◽  
R. Palomino-Merino ◽  
E. Moreno-Barbosa ◽  
E. Miguel-Chumacero ◽  
...  
Keyword(s):  
Plastic Scintillator

Underground Prototype Water Cherenkov Muon Detector with the Tibet Air Shower Array

2008 ◽  
Author(s):  
M. Amenomori ◽  
X. J. Bi ◽  
D. Chen ◽  
S. W. Cui ◽  
Danzengluobu ◽  
...  
Keyword(s):  
Muon Detector ◽  
Air Shower ◽  
Shower Array ◽  
Air Shower Array

DESIGN, PREPRODUCTION, AND PERFORMANCE OF THE CDF RUN IIB SILICON DETECTOR

2005 ◽  
Vol 20 (16) ◽  
pp. 3811-3814
Author(s):  
◽  
PAUL LUJAN
Keyword(s):  
Building Block ◽  
Silicon Detector ◽  
Radiation Hardness ◽  
Control Signals ◽  
Lightweight Structure ◽  
And Performance ◽  
Performance Results ◽  
And Control ◽  
Radiation Hard ◽  
Detector Design

A new silicon detector was designed by the CDF collaboration for Run IIb of the Tevatron at Fermilab. The main building block of the new detector is a "supermodule" or "stave", an innovative, compact and lightweight structure of several readout hybrids and sensors with a bus cable running directly underneath the sensors to carry power, data, and control signals to and from the hybrids. The hybrids use a new, radiation-hard readout chip, the SVX4 chip. A number of SVX4 chips, readout hybrids, sensors, and supermodules were produced and tested in preproduction. The performance (including radiation-hardness) and yield of these components met or exceeded all design goals. The detector design goals, solutions, and performance results are presented.

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